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European Quantum Electronics Conference (EQEC)

Zeeman effect for molecular rydberg states

V. E. Chernov, Dmitrii L. Dorofeev, B. A. Zon

Published Aug 24, 2005• 0 citations
Publisher
DOI
10.1109/eqec.1994.698431

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Journal of Physics B Atomic and Molecular Physics•Jul 28, 1984•3 citations
Rydberg states of the NO molecule have been probed by two-color resonantly enhanced multiphoton ionization in a magnetic field of 0.93 T. Penetrating s and d states show strong interactions with the intramolecular field while nonpenetrating f states show stronger interactions with the external magnetic field. Competition between the molecular core anisotropy and the external field anisotropy leads to a greater variety of situations than in a Rydberg atom, ranging from a “weak field” regime to a “strong field” regime. These different situations are illustrated by a multichannel quantum defect calculation on the np states of NO including the Zeeman effect. An extreme situation can be achieved in which the Rydberg molecule looses its molecular character and shows an almost pure atomic structure within each rotational channel.
We observe weakly-bound ΠΠΠ-symmetry electronic states in the spectroscopy of 87^{87}87Rb(nP3/2)(nP_{3/2})(nP3/2​)+87^{87}87Rb(5S1/25S_{1/2}5S1/2​) ultralong-range Rydberg molecules. We detect these molecules in Rydberg states having principal quantum number 13≤n≤1613\le n \le 1613≤n≤16. Their ΠΠΠ-state character is unambiguously identified via their observed multiplet structure: the 2F+12F+12F+1 magnetic sublevels of the ground-state rubidium atom separate, as in the Zeeman effect, because of the spin-spin coupling between the Rydberg and valence electrons. We find a rapid decrease in the molecular binding energy ∝(n−μP3/2)−11\propto (n-μ_{P_{3/2}})^{-11}∝(n−μP3/2​​)−11, where μP3/2μ_{P_{3/2}}μP3/2​​ is the quantum defect, indicating that the low-nnn regime of Rydberg states is ideally suited for studies of ΠΠΠ-symmetry molecules. Our observations are in good agreement with Green's function-based calculations for 14≤n≤1614\le n\le 1614≤n≤16, with poorer agreement for n=13n=13n=13 hinting at the beginning of a breakdown of the Fermi pseudopotential approach at low nnn.